The \(\vec{e}p \rightarrow e p \gamma \)  cross section in the DVCS regime was
recently measured by the Hall A collaboration at Jefferson
Laboratory (JLab) [1]}. The cross section involves the contributions
of the Bethe-Heitler (BH) amplitude squared, the DVCS amplitude squared and
the interference of the BH and DVCS amplitudes.
Based on the kinematics of the experiment,
in the analysis of the data,
the contribution of the DVCS amplitude squared was neglected compared to the other
two contributions [2]},
which allowed for the extraction of the so-called Compton
form factors of the proton.
